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Cranfield University

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Experimental Methods<br />

tyre, there is symmetry between the left (1, 2, 3) and the right (10, 9, 8) hand side of the<br />

soil bin with the highest values in the centre (five and six). Thus measurements taken at<br />

symmetrical positions relative to the centre of the rut have similar readings and conse-<br />

quently these readings were averaged resulting in the curves shown in Figure 17 b).<br />

The curves 4+7 and 5+6 in Figure 17 b) coincide so giving the possibility of averaging<br />

them and thus creating one penetrometer resistance curve per treatment representing the<br />

average of the centre 4 points of measurements or the centre 360 mm of the rut. This mean<br />

curve is shown in Figure 17 c). The same procedure was applied for the initial control.<br />

2.2.3 Dry Bulk Density<br />

Two different methods to determine dry bulk density were used. In the soil bin only a den-<br />

sity ring was utilized and in the field measurements both, a density ring and a gamma ray<br />

probe (Troxler) were used.<br />

2.2.3.1 Gravimetrical Density Measurement<br />

Dry bulk density (DBD) was measured gravimetrically at depths of 0, 250, and 500 mm,<br />

with three replications before and after each run, at the centre of the track mark in the soil<br />

bin. A cylindrical ring (60 mm diameter and 51.5 mm deep) was pushed into the soil and<br />

excavated. The surplus soil was carefully cut off and the soil sample from the cylinder<br />

weighed and dried for 48 h at 105 o C. The dry soil was weighed and soil water content<br />

determined from the weight difference. Dry bulk density was calculated from the given<br />

volume of the cylinder and the dry weight.<br />

2.2.3.2 Nuclear Density Measurement Gauge<br />

With the aim to gain a more precise resolution of the increase in soil density a nuclear den-<br />

sity gauge, namely a Troxler 3430, was used to measure soil density. With this measure-<br />

ment device a gamma source is positioned at a known depth in the soil in a previously cre-<br />

ated access hole. Once the gamma source is in position and switched to transmitting mode,<br />

the detectors located within the gauge count the received radiation, which depends on the<br />

dry bulk density and the depth of location of the source within the soil. From this the ma-<br />

Ph.D. Thesis Dirk Ansorge (2007)<br />

24

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